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Compare Description Drawings, CAD & Specs DiameterWavelength RangeMaterialSurface Quality Avail. Price
Broadband Beam Samplers10B20NC.125.4 mm440-700 nmGrade A N-BK715-5 scratch-dig
$112
Broadband Beam Samplers10B20NC.225.4 mm660-1000 nmGrade A N-BK715-5 scratch-dig
$124
Broadband Beam Samplers10B20NC.325.4 mm1010-1550 nmGrade A N-BK715-5 scratch-dig
$135
Broadband Beam Samplers10Q20NC.125.4 mm440-700 nmUV Grade Fused Silica15-5 scratch-dig
$130
Broadband Beam Samplers10Q20NC.225.4 mm660-1000 nmUV Grade Fused Silica15-5 scratch-dig
$141
Broadband Beam Samplers10Q20NC.325.4 mm1010-1550 nmUV Grade Fused Silica15-5 scratch-dig
$151
Broadband Beam Samplers10Q20NC.UV25.4 mm255-440 nmUV Grade Fused Silica15-5 scratch-dig
$201
Broadband Beam Samplers10Q40NC.125.4 mm440-700 nmUV Grade Fused Silica10-2 scratch-dig
$306
Broadband Beam Samplers10Q40NC.225.4 mm660-1000 nmUV Grade Fused Silica10-2 scratch-dig
$317
Broadband Beam Samplers10Q40NC.325.4 mm1010-1550 nmUV Grade Fused Silica10-2 scratch-dig
$333
Broadband Beam Samplers20B20NC.150.8 mm440-700 nmGrade A N-BK715-5 scratch-dig
$224
Broadband Beam Samplers20B20NC.250.8 mm660-1000 nmGrade A N-BK715-5 scratch-dig
$253
Broadband Beam Samplers20B20NC.350.8 mm1010-1550 nmGrade A N-BK715-5 scratch-dig
$279
Broadband Beam Samplers20Q20NC.150.8 mm440-700 nmUV Grade Fused Silica15-5 scratch-dig
$302
Broadband Beam Samplers20Q20NC.250.8 mm660-1000 nmUV Grade Fused Silica15-5 scratch-dig
$318
Broadband Beam Samplers20Q20NC.350.8 mm1010-1550 nmUV Grade Fused Silica15-5 scratch-dig
$333
Broadband Beam Samplers20Q20NC.UV50.8 mm255-440 nmUV Grade Fused Silica15-5 scratch-dig
$412
Broadband Beam Samplers20Q40NC.150.8 mm440-700 nmUV Grade Fused Silica10-2 scratch-dig
$488
Broadband Beam Samplers20Q40NC.250.8 mm660-1000 nmUV Grade Fused Silica10-2 scratch-dig
$501
Broadband Beam Samplers20Q40NC.350.8 mm1010-1550 nmUV Grade Fused Silica10-2 scratch-dig
$515
Broadband Beam Samplers580125.4 mm350-2000 nmGrade A N-BK720-10 scratch-dig
$144
Broadband Beam Samplers580250.8 mm350-2000 nmGrade A N-BK720-10 scratch-dig
$235

Specifications

  • Angle of Incidence
    45°
  • Damage Threshold
    500 W/cm2 CW, 1.0 J/cm2 with 10 nsec pulses, typical
  • Surface Flatness
    ≤λ/10 at 632.8 nm over the clear aperture
  • Diameter Tolerance
    +0/-0.13 mm
  • Wedge
    30 ±15 arc min
  • Clear Aperture
    > central 80% of diameter
  • Chamfers
    0.25-0.76 mm face width
  • Chamfers Angle Tolerance
    45° ±15°
  • Durability
    MIL-C-675C, moderate abrasion million cycles
  • Cleaning

Features

Fresnel Reflection

A material that exhibits birefringence, or different refractive indices for different input polarizations, is said to be anisotropic. This anisotropy affects the transmission and absorption properties of light and is the primary mechanism used in polarizers and waveplates. However, even isotropic materials (same index for different polarizations) can enable polarization selection via reflection. For a linearly polarized beam, both S- and P-polarizations exhibit different changes in reflectivity versus incident angle. There is an incident angle known as Brewster’s angle (θB) at which P-polarized light is transmitted without loss, or exhibits zero reflectance, while S-polarized light is partially reflected. This angle can be determined from Snell’s law to be θB = arctan(n2/n1). The accompanying figure shows this response when light is incident from air onto a dielectric material where θB ≈ 56°.

Broadband Beam Samplers

In a beam sampler, the percentage of reflected light is determined by the Fresnel reflection from a single surface. By reflecting approximately 10% of S-polarization and 1% of P-polarization at the nominal 45° AOI, the beam sampler picks off 1-10% of an incident beam, depending on its polarization upon incidence. Reflectance from a single uncoated surface for both S- and P- polarizations is shown here. The graph exhibits reflectance of the plate as a function of incident angle, showing the minimum in the P-polarization at Brewster’s angle, 55° 34’.

N-BK7 Substrates for VIS and NIR Applications

N-BK7 is an excellent lens material for general use such as most visible and near infrared applications. It is the most common borosilicate crown optical glass, and it provides great performance at a good value. Its high homogeneity, low bubble and inclusion content, and straightforward manufacturability make it a good choice for transmissive optics.

UV Fused Silica for UV & Broadband Applications

UV Grade Fused Silica is synthetic amorphous silicon dioxide of extremely high purity providing maximum transmission from 195 to 2100 nm. This non-crystalline, colorless silica glass combines a very low thermal expansion coefficient with good optical qualities, and excellent transmittance in the ultraviolet region. Transmission and homogeneity exceed those of crystalline quartz without the problems of orientation and temperature instability inherent in the crystalline form. It will not fluoresce under UV light and is resistant to radiation. For high-energy applications, the extreme purity of fused silica eliminates microscopic defect sites that could lead to laser damage.

Slight Wedge Suppresses Unwanted Fringes

Optics with perfectly parallel faces are unsuited for use as reference elements in laser setups as reflections from both surfaces would be collinear resulting in undesired large period fringes. The introduction of a slight wedge causes unwanted reflections from the second surface to be deflected from the optical path. The back surface (S2) of these beam samplers is slightly wedged. The laser beam should enter the non-wedged surface (S1) where an arrow on the side points to.

AR Coated Back Surface Eliminates Ghosting

An antireflection coating of high damage threshold (500 W/cm2 CW, 1.0 J/cm2 with 10 nsec pulses, typical) is applied on the back surface (S2) to minimize ghost reflections. Four broadband AR coatings are offered and optimized for 45° angle of incidence beams with <0.75% reflectance. NC.1 covers the 440-700 nm spectral range, NC.2 covers the 660-1000 nm spectral range, NC.3 covers the 1010-1550 nm spectral range and NC.UV covers the 255-440 nm spectral range. Uncoated version is also available, used as beam pick-off optics, to monitor the laser beam, independent of wavelength.

Laser Cavity Applications

Polarization-selective reflectivity is exploited in laser cavities to produce strongly polarized light, as well as for fine tuning of the output laser wavelength. A Brewster’s window is used in the laser cavity, providing polarized light output with minimal power loss. It follows the formula θB = arctan(n), where θB is Brewster’s angle and n is the index of refraction of the material. Often, fixed beam polarization is necessary in order that optical components can consistently perform as they were designed.

Power Measurement Applications

A common application for beam samplers is picking off a portion of a beam in order to track changes in beam power vs time using a detector. This information may be used as part of a feedback loop to regulate power, or could simply be used to log power in order to normalize experimental results at a later time. For measuring beam power, the beam sampler should be oriented such that the laser is p-polarized. This choice will maximize transmitted power and attenuate power incident on the detector.

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